US 7515269 B1
A method of particle detection includes optically trapping a single particle having an averaged linear dimension of between 0.10 microns and 50 microns in a focal region optical trap formed from a trap visible to near-infrared wavelength. The trap is proximal to a substrate having a discontinuous metal coating so as to exploit a surface plasmon resonance generated electric field caused by irradiation of the metal coating. The single particle is then exposed to an interrogation wavelength to yield scattering spectrum relating to the particle. A particle identification digital database containing scattering spectra from a variety of different single particles that vary in spectral features facilitates identification of unknown spectra. A microfluidic cell is detailed to facilitate the automated scanning of numerous particles from a sample.
1. A method of particle detection comprising:
optically trapping a single particle having an averaged linear dimension of between 0.10 microns and 50 microns in a focal region optical trap formed from a visible to near-infrared trap wavelength, said trap being proximal to a substrate having thereon a discontinuous metal coating that generates a plasmon electric field upon irradiation by an interrogation wavelength;
exposing said single particle to the interrogation wavelength thereby producing a scattering spectrum relating to said particle and enhanced by said plasmon electric field; and
collecting the scattering spectrum relating to said particle.
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This application is a utility application claiming priority of U.S. provisional application 60/541,398 filed Feb. 3, 2004.
The invention described herein may be manufactured, used, and licensed by or for the United States Government.
This invention in general relates to a method and system for particulate optically trapped SERS characterization and in particular, to a method and system for non-destructive single particle characterization.
Particulate analyte characterization is currently limited to averaging techniques that sample a field of particles under comparatively mild sampling conditions, or single particle interrogation techniques that subject the particle to a harsh sampling condition in order to generate a sufficient signal relative to background noise. Unfortunately, many forms of particulate, including organic polymers and biological cells cannot tolerate the spectroscopic techniques needed to characterize them directly. Instead, one resorts to staining or shadowing techniques that are both labor intensive and destructive of the test subject. The time required to characterize particulate also limits the use of such information in rapidly changing situations as diverse as a manufacturing, treating an infection, and managing a contamination event.
Accurate and sensitive detection of viruses and hazardous microorganisms is a requirement in numerous industrial, military, workplace, healthcare and even home environments. A difficulty that arises in biological detection is the relative paucity of molecules that are exclusively found in targets. Additionally, the inability of a single technique to afford definitive characterization through the strain level of the microbe means that culturing the sample is often required thereby increasing the time-consumed in characterization. Animate particulate, such as that found in a forensic setting, simply is not fully characterized.
Since the seminal work of Ashkin in 1970, based on a dual laser beam system (1) and later work in 1986 employing a single laser beam apparatus (2), the laser tweezer phenomenon has been broadly accepted as a powerful tool to study viruses (3), vegetative bacterial cells (4-8), mammalian cells (9) and colloidal crystallization in microgravity environments (10). More recently, this technique in combination with various Raman detection schemes has been applied to the investigation of inorganic gas bubbles (11), aerosols (12), emulsion particle polymerization (13), liquid-liquid extraction of toluene in water (14), organic nanoparticles (15), yeast cells (8) and solid-phase peptide synthesis (16).
Raman spectroscopy has been an invaluable technique in the study of various chemical systems and has become widely accepted as an analytical characterization methodology (17,18). The attractiveness of this technique stems from the attributes of narrow spectral band structure, lack of interference from water, and relative insensitivity to the excitation wavelength employed. However, un-enhanced Raman spectral features are considered to be relatively weak thus requiring relatively lengthy collection times. In many applications, high quality spectra may be achieved with shortened acquisition times and improved spectral features by exploiting various amplification techniques. Namely, Resonance Raman Scattering (RRS), Surface Enhanced Resonance Raman Scattering (SERRS) or Surface-Enhanced-Raman-Scattering (SERS) (17-19). RRS and SERRS are typically conducted using ultraviolet excitation to facilitate electronic excitation (i.e. strong absorption) in the analyte of interest. Ultraviolet excitation precludes implementation of RRS and SERRS in a single beam optical trapping configuration since the trapped particle experiences MW/cm2 UV intensity levels that coupled with significant UV-light absorption photo-decompose most analytes.
SERS represents another method for enhancing a conventional Raman signal that is operative with less destructive near-infrared optical beam trapping. Currently, the mechanism of the SERS effect is not fully understood; however, a plausible explanation for at least a significant portion of the spectral amplification has been attributed to an increase in the electromagnetic field strength encountered by the analyte. Briefly, this intensified electromagnetic field is generated when a roughened metal surface (typically, Au, Ag, Pt, Pd or Cu) is irradiated with the requisite wavelength of light and metal conduction band electrons are excited to collective oscillation and produce a surface plasmon resonance. The Raman and infrared (IR) signals associated with analytes proximal to such a metal surface have been shown to be enhanced from 4 to 14 orders magnitude relative to un-enhanced Raman (17). Additionally, the enhancement is reversible when the particulate analyte is removed from the metal surface. In spite of these features, SERS has gained only limited acceptance since early reports on this technique in the late 1970's. This limited acceptance is in large part due to the lack of fabrication reproducibility in most SERS substrates. Relatively recent advances in SERS-active substrate fabrication have addressed this reproducibility issue. Specifically, these substrates are easily wavelength adjustable, durable, biocompatible and possess a long shelf-life (19).
Bacterial spore characterization is a subset of particulate characterization where the limitations of current techniques are profound. Endospores are an alternate cell form of various bacterial genera including Bacillus, Clostridium, Desulfotomaculum, Oscillospira, Sporosarcina, Sporolactobacillus, and Thermoactinomyces. An endospore is formed as an adaptive response to environmental conditions unfavorable to the bacterial cell form, such as dehydration, limited nutrient availability and extreme temperatures. While endospores are themselves metabolically inactive, they are activated under appropriate conditions, forming an active vegetative bacterial cell. Thus, the presence of an endospore is indicative of a potential biohazard and therefore endospore detection is a desirable goal.
Over the past three decades Raman spectroscopy has been employed to study various Bacillus spore species. Due to the relatively meager Raman scattering cross-sections exhibited by many biological materials, a majority of this reported work has been conducted using various Raman amplification techniques. Specifically, early work in this area was based on the Resonance-Raman-Scattering (RRS) technique utilizing ultraviolet (i.e., 222 nanometer) to green (i.e., 514.5 nanometer) laser excitation sources (20-23). More recently, reports have been published describing the implementation of Femtosecond Adaptive Spectroscopic Techniques applied to Coherent-Anti-stokes-Raman-Spectroscopy (FAST CARS) (24) as well as SERS microscopy (25). These various Raman spectroscopies have been applied to the study of bulk endospore samples and have failed to afford information sufficient to distinguish between strains of the same endospore.
Thus, there exists a need for a non-destructive characterization technique for single particles. The ability to characterize a single particle in a non-destructive manner confers the ability to examine particulate changes over time and to assess population diversity.
A method of particle detection includes optically trapping a single particle having an averaged linear dimension of between 0.10 microns and 50 microns in a focal region optical trap formed from a trap visible to near-infrared wavelength. The trap is proximal to a substrate having a discontinuous metal coating so as to exploit a surface plasmon resonance generated electric field caused by irradiation of the metal coating. The single particle is then exposed to an interrogation wavelength to yield scattering spectrum relating to the particle.
A particle identification system is provided that includes a digital database containing scattering spectra from a variety of different single particles that vary in spectral features. An algorithm applies a chemometrics protocol to an unknown particle spectrum to determine the relationship between the unknown particle spectrum and one or more standards spectra from the database. A computer is provided to run the algorithm and access the database. A user interface is coupled to the computer for manual data entry. A particle identification system is particularly well suited for endospore particles since the genealogy of a virulent endospore is critical in rapidly identifying the source of the outbreak.
A microfluidic cell is detailed to facilitate the automated scanning of numerous particles from a sample. The cell includes a vessel having a spectroscopic sampling region defined by a wall. The spectroscopic sampling region has a sampling cross sectional dimension and is transmissive to at least one of ultraviolet, visible, and near infrared radiation. The sampling region is in fluid communication with a sample buffer region that has a larger cross sectional dimension than the sampling cross sectional dimension. A discontinuous metal coating is applied to the backwall of the spectroscopic sampling region. A fluid injector drives a fluid from the buffer region to the sampling region until a particle is detected within the sampling region. This process is repeated to scan numerous single particles in an automated fashion. A statistically meaningful characterization of the total sample is achieved in this manner.
The present invention has utility in the detection of single particles or a solvent volume under conditions that are unlikely to impair biological particle viability or modify inanimate particle chemical properties. The present invention in providing a spectroscopic fingerprint of a single particle has utility in settings illustratively including food processing and medical diagnosis where the presence of particular bacteria, endospores, or viruses are indicative of contamination or infection; manufacturing process control of particulate materials; biohazard monitoring and response; reaction monitoring of particle reaction in the presence of possible reactants; intra-particle morphological change mechanisms; and forensic investigations as to the origin of a particle.
Collection of a scattering spectrum from a single particle is enhanced by spectrum collection in proximity to a discontinuous metal coating that generates a surface plasmon resonance signal upon irradiation. Through adjustment of the distance between the particle and the discontinuous metal coating, the spectrum collected is representative of different portions of the particle thereby allowing the collection of surface weighted spectra, as compared to a particle volume averaged spectrum. Distance adjustment between the discontinuous metal coating and the optical trap is most easily performed through supporting the substrate on a microscope stage and moving the stage relative to the optical trap. Alternatively, the optical trap is translated with an optical tweezers.
As used herein “particle” or “particulate” are synonyms defined to include a domain distinct from a surrounding solvent and having an averaged linear dimension over the three orthogonal axes of between 0.10 and 50 microns for a single domain or an aggregate domain. A particle suitable for spectral interrogation according to the present invention illustratively includes a eukaryotic cell, a bacterium, a virus, a polymer strand, an organelle, a colloid, and a nanocrystal. While an individual particle is routinely suspended alone in an optical trap for spectral investigation, it is appreciated that a particle can be adhered to the surface of another type of particle to adjust the average linear dimension. By way of example, a virus particle or multiple virus particles can be adhered to a colloidal particle surface or a target cell and the resulting aggregate particle is amenable to spectral interrogation according to the present invention. Colloidal silica is particularly well suited for aggregate particle formation. Likewise, ribosomes, antibodies, or nanocrystals having an average linear dimension of less than 0.10 microns are adhered to a colloidal particle surface by conventional techniques. These techniques include the use of an intermediate coupling agent such as biotin, thiols, epoxides, and organosilanes.
According to the present invention, an optical trap is formed in the focal region of a microscope objective with visible or near-infrared laser light to maintain a particle within the trap volume. Through the use of a translation stage, an optical trap functions as optical tweezers, allowing the movement of a trap relative to the point of trap formation. Optical tweezer physics and properties are well known (2). The near-infrared optical tweezers are combined with an incident interrogation wavelength that is used to generate a scattering spectrum from the particle in proximity to a discontinuous metal surface.
A preferred component schematic for performing an inventive method of particle detection is shown in
Both Rayleigh and inelastic scattered light (dashed line) 32 from the single, trapped particle 26 is collected by the same 100× oil immersion objective 24 and collimated onto and directed by the dichroic mirror 28 through the holographic filter 12, an intermediate mirror 34, a second holographic filter 36 before being focused by a lens 37 onto the entrance slit of a 0.275 meter polychromator 38 (SpectraPro®-275, Acton Research Corporation) and liquid nitrogen-cooled, back illuminated charge coupled device (CCD) 40 (Spec-10:100BR, Roper Scientific) for spectral analysis. The holographic filters have optical densities better than 6.0 so as to remove the majority of Rayleigh scattering. The scattered light 32 is enhanced by placing the sample 26 in proximity with a discontinuous metal coating 41. Light 32 coupled into the polychromator 38 is laterally dispersed across the 1340×100 pixel CCD 40 by a 1200 groove/mm grating (not shown) within the polychromator 38, the grating is blazed at 750 nanometers. The polychromator 38 is controlled through a digital-to-analog converter 42 and data is collected from the CDD 40 by a personal computer 44 though a 16-bit interface card (not shown) using the WinSpec/32™ software package (Version 220.127.116.11, Roper Scientific). To increase the signal to noise (S/N) ratio the output of the CCD 40 is vertically binned prior to readout. The area immediately surrounding the optical trap in the sample 26 is imaged through the microscope objective 24 and imaging optics 46 (Edmund Industrial Optics) by a near infra-red-sensitive video camera 48 (NEC TI-24A). A reflective neutral density filter 50 is placed before the camera 48 to further reduce the amount of laser light reaching the camera. Images from this video camera 48 are displayed on a video monitor 52 for observation and digitized for later inspection using an 8-bit analog-to-digital framegrabber 54 (PixelSmart, Lewiston N.Y.).
The schematic of
For surface-enhanced Raman scattering, the interrogation light source is selected to generate radiation having a wavelength that causes appreciable Raman-scattering in the presence of the particle being measured. Although it is known that Raman-scattering occurs essentially at all wavelengths, preferably, the radiation employed is near-infrared radiation since ultra-violet radiation is associated with parasitic fluorescence. Typically interrogation wavelengths range from 320 to 1700 nanometers. Preferred interrogation wavelengths range from 650 to 1100 nanometers. Laser diodes are commercially available to select numerous specific laser lines within the preferred interrogation wavelength range. It is appreciated that longer wavelengths such as 1064 nanometers are operative herein provided that a InGaAs detector is employed. This detector is operative to 1700 nanometers.
A discontinuous metal coating has a high surface area to volume ratio and is fabricated on a surface of the substrate by conventional means including, for example, magnetron sputtering, plasma sputtering, and electron-beam evaporation. The metal is selected to create a large diameter surface plasmon resonance electric field under illumination by either the trap wavelength or the interrogation wavelength. Discontinuous metal coatings are illustratively formed from gold, silver, platinum, palladium, copper, and alloys thereof. The coating typically has an average thickness of about 0.02 micron to 2 microns and preferably about 0.02 microns to 0.5 micron. Electrically conductive colloidal material is readily synthesized from gold, silver, platinum, palladium, copper, and alloys thereof by reduction of aqueous metal salts in the presence of a passivating ligand or a coordinating solvent or etching of a uniform film to for a nanoporous coating. Alternatively, carbon or silica grains coated with the electrically conductive material. The electrically conductive colloidal material typically has an averaged linear dimension over the three orthogonal axes ranging from 10 to 10,000 nanometers and preferably from 30 to 100 nanometers.
Additives that are operative herein illustratively include a second particle that is the same or different than the single particle, a reactant towards the single particle, a metabolite of the single particle, and a toxin towards said single particle. The case of a bacterium or an endospore the presence of another cell or virus is effective in observing if there is inter-cellular communications to trigger a change in the single particle. Additionally, besides the inter-cellular exchange of messenger molecules, cells are known to emit compounds cytotoxic to all, but closely related cells. Such observations are helpful developing treatments and lysis mechanisms against pathogenic cells. The value of studying the effect a given molecular reactant has on a particle is not confined to biological cells, conformational or electrical changes associated with polymer strands; inorganic platelets, such as bentonite clays, and magnesium hydroxide; semiconductor nanocrystals, and other systems represents a valuable research and quality control function. By way of example, the introduction of a silver metal ion serving as a surface trap quencher would be observed in the SERS spectrum of a 100 nanometer CdSe nanocrystal.
In some situations, it is desirable to detect particles such as bacterial endospores in environments other than those found or maintained at room temperature. For example, it may be of interest to detect bacterial endospores in cold storage compartments, or in heated facilities or reaction chambers. In such cases a suitable solvent is selected that has a melting temperature such that the solvent is in the liquid state at the ambient temperature in the environment to be tested. Suitable solvents for extreme temperature range spectroscopy according to the present invention are well known to the art and illustratively include glycols; glymes; ionic liquids; liquefied gases such as nitrogen; and alcohols. Through appropriate choice of solvent, particles can be detected according to the present invention in the range between −200 to 200 degrees centigrade.
An environmental sample is needed to produce a sample containing a single particle. An environmental sample is in any of various forms such as a gas, an aerosol, a liquid, a solid and a suspension. Methods of obtaining environmental samples are known and include such techniques as dry swabbing, wet swabbing, filter collection, impinging of an air or aerosol from the environment to be tested onto a surface for particle capture, such as a solid, liquid or gel capture surface. An example of such a particle capture surface is a gelatin-coated laboratory slide. An environmental sample is optionally acquired over a specified period of time, for example to facilitate identification of a contaminating incident. In a further option, the environmental sample is representative of a specified location of the environment to be tested, so as to facilitate decontamination of the location. In addition, the environmental sample optionally represents a specified portion of the environment, so as to facilitate calculation of the total particle quantity.
In order to transfer a particle from an environmental sample to an optical trap for sampling, the sampling solvent and environmental sample are brought into contact. For example, where an environmental sample is a dry swab of the environment to be tested, the swab may be brought into contact with the sampling solvent, such as by immersion for a suitable time. A suitable time may be determined by using standards with known concentrations of a particle, so as to calibrate the operation of the method under specific conditions.
The accurate transfer of any or all of the particulate within an environmental sample to optical traps for spectroscopic scattering experiments is facilitated through the use of a microfluidic cell as shown generally at 80 in
In use, an environmental sample is solvated with a measured quantity of the trap solvent and the solvent loaded into a sample reservoir 96. The sample reservoir volume is metered through the filter 94 into the buffer region 92 into the sampling region 82 by a fluid injector 98. Upon priming the buffer region 92 single particles can be seized within an optical trap and successively scanned. While the fluid injector can be as simple as a manual micropipette, a capillary electro-osmotic pump is preferred. A capillary electro-osmotic pump draws particles having a charge in an appropriate buffer through a capillary fiber having an electrical bias. In this way continuous particle supply is drawn to the sampling region 82 so that the optical train can be maintained in a continual operational mode. A suitable capillary electrophoresis system is available from Agilent Technology that is adaptable for use as a capillary electro-osmotic pump. The system is amenable to automation so that a statistically significant number of single particles can be spectroscopically scanned. Automation is facilitated by image analysis software that identifies a particle within the optical trap volume imaged by a video camera in
A collection of spectra from a variety of particles is readily assembled into a standards database. In addition to the spectra from a given particle, preferably the database also stores characterization information about the particle such as collection specifics, cross-references to characterization derived from other techniques, and images collected through the microscope optics during the scattering experiment. The different spectra in the database are compared to an unknown spectrum for characterization and to identify overlap between the unknown and standards within the database. The digital storage of spectra facilitates computational normalization and comparison routines. With an inexact match between an unknown spectrum and at least one record found in the standards database, the extent of relatedness is preferably determined with an chemometric algorithm such as a neural network, or Principle Component Analysis (PCA) (30-34). This is especially effective in the instance of particles of biological origin, where evolutionary changes such as mutations are noted as populations diverge. A computer is provided to run the algorithm and access the database. A user interface to the computer and database allows for manual data entry and the manipulation of data as part of a standards fitting routine. Optionally, the database is centralized and remote from the computer and access in via an intranet or the Internet. Preferably, a user has the option to add a new unknown spectrum to the centralized database, such that a subsequent user of the database may be able the provide information about the unknown spectra. A standard fit to the unknown by a subsequent user can trigger notification to the unknown submitter. A standards database is particularly well suited for endospore particles since the genealogy of a toxic endospore is critical in rapidly identifying the source of the outbreak.
The present invention is further detailed with respect to the following non-limiting examples. These examples are intended only to illustrate particular aspects of the invention and in no way limit the scope of the appended claims.
SERS-active substrates are prepared by a method similar to that suggested by Grabar, Freeman, Hommer and Natan (19) using freshly synthesized 60 nanometer gold colloids. Briefly, standard glass microscope slides are cleaned for 1-h in a bath consisting of 1:4 (v/v) 30% H2O2 to sulfuric acid bath at 60° C. Subsequent to cleaning, the microscope slides are profusely washed in methanol and stored in fresh CH3OH until needed. A self-assembled-monolayer (SAM) of 3-Aminopropyltriethoxy silane (APTES; Aldrich Chemical Company) is formed on the cleaned glass substrates by submerging the glass slides in a solution of the silane diluted 1:4 (v/v) in methanol. After 24-h, the APTES-derivatized glass is removed from the silane solution and washed repeatedly (˜15×) with methanol to remove any unbound silane from the surface. The APTES-derivatized glass is stored in fresh methanol until needed.
Gold colloids of 60 nanometer size freshly prepared by a previously published (26) method are coupled to the silanized substrate by immersing the washed glass in the aqueous colloidal suspension for 24-h at room temperature. Subsequent to the colloidal coupling the SERS substrates are washed with and stored in de-ionized water until needed for analysis. UV-visible absorbance measurements (not shown) of these substrates reveal a Surface Plasmon Resonance (SPR) optimally excited with 715 to 775 nanometer light. SERS-substrates fabricated through this method are near optimally excited using the NIR-RTDS.
Bacillus stearothermophilus (ATCC 10149 and ATCC 7953) are purchased from Raven Biological Laboratories, Inc. (Omaha, Nebr.) as 40% ethanol-deionized water suspensions. According to the manufacturer, these spores were prepared by incubation in soybean-casein digest broth at 55 to 60° C. for 7 days. Samples for measurement are prepared by diluting 100 microliters of the spore suspension in 40 milliliters of 18 MΩ deionized water to give a final concentration of 7.5×104 CFU/ml (CFU=colony forming units).
A series of spectra are collected with a laser excitation power of 20-mW (before the microscope), 500-ms integration, 100 co-additions at a spectral resolution of 7.5 cm−1 unless otherwise stated using the system described with respect to
The performance of the near-infrared Raman-Tweezer Detection System (NIR-RTDS) of
The SERS spectral differences between the Bacillus stearothermophilus endospores studied are more apparent in
Any patents or publications mentioned in this specification are indicative of the levels of those skilled in the art to which the invention pertains. These patents and publications are herein incorporated by reference to the same extent as if each individual publication was specifically and individually indicated to be incorporated by reference
One skilled in the art will readily appreciate that the present invention is well adapted to carry out the objects and obtain the ends and advantages mentioned, as well as those inherent therein. The present methods, procedures, treatments, molecules, and specific compounds described herein are presently representative of preferred embodiments, are exemplary, and are not intended as limitations on the scope of the invention. Changes therein and other uses will occur to those skilled in the art which are encompassed within the spirit of the invention as defined by the scope of the claims.